String bordism

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(The String group)
(The String group)
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== The String group ==
== The String group ==
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There are various models for the String group. Since its first three homotopy groups vanish it can not be realized as a finite dimensional Lie group. There are homotopy theoretic constructions which use loop space constructions, that is, inifnite dimensional techniques. A more geometric way to think about $String(n)$ is the following: the String group fibers over the Spin group with fibre $K({\mathbb Z},2)$. One may think of $ K({\mathbb Z},2)$ as the realization of the finite dimensional Lie groupoid $S^1$ viewed as a category with only one object. This way, the String group as an $A_\infty$-space appear as the realization of a smooth extension of $Spin(n)$ by the finite dimensional Lie groupoid $S^1$ (see \cite{Schommer-Pries2010}). A more explicit model for this extension can be found in \cite{Meinrecken03}.
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There are various models for the String group. However, since its first three homotopy groups vanish it can not be realized as a finite dimensional Lie group. There are homotopy theoretic constructions which involve path spaces, that is, inifnite dimensional techniques. A more geometric way to think about $String(n)$ is the following: the String group fibers over the Spin group with fibre $K({\mathbb Z},2)$. One may think of $ K({\mathbb Z},2)$ as the realization of $S^1$ viewed as a smooth category with only one object. This way, the $A_\infty$ space $String(n)$ appears as the realization of a smooth extension of $Spin(n)$ by the finite dimensional Lie groupoid $S^1$ (see \cite{Schommer-Pries2010}). An explicit model for this extension can be found in \cite{Meinrecken03}.
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</wikitex>
</wikitex>

Revision as of 15:37, 31 March 2011

This page has not been refereed. The information given here might be incomplete or provisional.

Contents

1 Introduction

String-bordism or O\!\left< 8 \right>-bordism is a special case of a B-bordism. It comes from the tower of fibrations below.

\displaystyle  \xymatrix{BO\!\left< 8 \right>\ar[d] & \\ BSpin \ar[d]\ar[r]^{p_1/2}&K({\mathbb Z},4) \\ BSO\ar[d]\ar[r]^{w_2}& K({\mathbb Z}/2,2) \\ BO\ar[r]^{w_1}& K({\mathbb Z}/2,1) }

In each step the lowest homotopy group is killed by the map into the Eilenberg-MacLane spaces. In particular, BO\left< 8 \right> is the homotopy fibre of the map from BSpin given by half of the first Pontryagin class. The name String-group is due to Haynes Miller and will be explained below.


2 The String group

There are various models for the String group. However, since its first three homotopy groups vanish it can not be realized as a finite dimensional Lie group. There are homotopy theoretic constructions which involve path spaces, that is, inifnite dimensional techniques. A more geometric way to think about String(n) is the following: the String group fibers over the Spin group with fibre K({\mathbb Z},2). One may think of K({\mathbb Z},2) as the realization of S^1 viewed as a smooth category with only one object. This way, the A_\infty space String(n) appears as the realization of a smooth extension of Spin(n) by the finite dimensional Lie groupoid S^1 (see [Schommer-Pries2010]). An explicit model for this extension can be found in [Meinrecken03].

3 Low dimensional generators

The following computations of \Omega_*^{String} for * \leq 16 comes from [Giambalvo1971, p. 538].

  • For i \leq 6 the natural map \Omega_i^{fr} \to \Omega_i^{String} is an isomorphism. See framed bordism for these groups.
  • \Omega_7^{String} = 0.
  • \Omega_8^{String} \cong \Zz \oplus \Zz/2, generated by the exotic 8-sphere for the 2-torsion and a certain Bott manifold: see [Laures2004].
  • \Omega_9^{String} \cong \Theta_9/bP_{10} \cong (\Zz/2)^2, generated by exotic 9-spheres.
  • \Omega_{10}^{String} \cong \Zz/6, generated by an exotic 10-sphere.
  • \Omega_{11}^{String} = 0.
  • \Omega_{12}^{String} \cong \Zz, generated by a 5-connected manifold with signature 8 \times 992.
  • \Omega_{13}^{String} = 0.
  • \Omega_{14}^{String} \cong \Zz/2, generated by the exotic 14-sphere.
  • \Omega_{15}^{String} \cong \Zz/2, genreated by the exotic 15-sphere.
  • \Omega_{16}^{String} \cong \Zz^2.

4 Homology calculations

4.1 Singular homology

4.2 $K(1)$-local computations

4.3 $K(2)$-local computations

4.4 Computations with respect to complex oriented theories

The additive structure of the bordism groups is not fully determined yet. Clearly, since BO\!\left< 8 \right> is 7-connected the first 6 bordism groups coincide with the framed bordism groups. It is known that only 2 and 3 torsion appears (see [Giambalvo1971]). Indeed, localized at a prime p>3, string bordism splits additively into a sum of suspensions of BP, although the ring structure is different (see [Hovey2008]). The first 16 bordism groups has been computed by Giambalvo, at the prime 3 the first 32 bordism groups can be found in [Hovey&Ravenel1995]. Further calculations have been done in [Mahowald&Gorbounov1995].


5 The structure of the spectrum



6 The Witten genus

At the end of the 80s Ed Witten were studying the S^1-equivariant index of the Dirac operator on a loop space of a 4k-dimensional manifold. For compact manifolds a Dirac operator exists if the manifold is Spin. For the loop space LM this would mean that
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is String. Witten carried the Atiyah-Segal formula for the index over to this infinite dimensional setting and obtained an integral modular form of weight k. Nowadays this is called the Witten genus (see [Segal1988].)

The Witten genus can be refined to a map of structured ring spectra

\displaystyle W: MString \longrightarrow TMF

from the Thom spectrum of String bordism to the spectrum TMF of topological modular forms ([Ando&Hopkins&Rezk2006]). This map is also called the \sigma-orientation and is 15-connected (see [Hill2008]). The spectrum TMF was developed by Mike Hopkins and Haynes Miller (see [Hopkins2002].) It is supposed to play the same role for String-bordism as KO-theory does for Spin-bordism. Its coefficients localized away from 2 and 3 are given by the integral modular forms. The map W gives characteristic numbers which together with KO and Stiefel-Whitney numbers are conjectured to determine the String bordism class. Moreover, tmf is supposed to be a direct summand of MString as the orientation map W is shown to be surjective in homotopy (see [Hopkins&Mahowald2002].)


7 Characteristic numbers and index theory

References

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